CYANA Command: enoe reff: Difference between revisions

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== Parameters ==
== Parameters ==


; normalize=''integer'': (default: ''none'')
; b0field =''real'': (default: ''none'')
; normed =''integer'': (default: ''none'')
; tauc =''real'': (default: ''none'')
; rhoavg =''real'': (default: ''none'')
; time =''string'': (default: ''none'')


== Description ==
== Description ==


This command initializes the eNORA routine, fits the diagonal decays to obtain the auto-relaxation (rho) values and I(0), normalizes the cross peak intensities and fits the experimental buildups.
This converts the calculated cross-correlation rates to distances.


The diagonal peak to use for normalization is specified by the parameter '''normalize''', using the integers 1 or 2, with the integers referring to the proton dimension in the peak list.
There are two different approaches to determine spin-diffusion contributions to cross-peak buildups, both of which require PDB coordinates of a previously determined structure (a conventional NMR structure or an X-ray structure). Usually the lowest energy model of structure bundles is used for spin-diffusion calculation; however, averaging of spin-diffusion over individual conformers is possible, depending on how many structures were read, see
The parameter '''normed''' specifies, if one wants to keep non-normalizable peaks (0) or only peaks that are properly normalized (1).  


In practice, many diagonal peak decays cannot be fitted (due to spectral overlap, artifacts, etc.):
The parameter '''mode''' is used to select the spin diffusion correction method (FRM:1, TSS: 2).
The parameter '''rhoavg''' allows the input of an average auto-relaxation values to be used non specifically [s-1].  
For the full-matrix (FRM, mode=1) approach to spin-diffusion approximation we use the multi-spin Solomon equation to express the mixing time-dependence of the NOESY intensities. In the FRM approach, the buildup intensities containing spin-diffusion are calculated for all spins within the spheres centered at spins i and j (Orts et al. 2012).


A spin-type specific value may be calculated to be read in a file containing spin type specific auto-relaxation values, the same file may be used to read spin-type specific I(0) values,
see * [[CYANA Command: read rho|read rho]].


The parameter '''time''' specifies the measured NOE mixing times in ascending order [s]. The NOE mixing times are given as a coma separated list, i.e. time="0.02,0.04,0.06"
In the TSS (TSS, mode=2) approach, we follow a strategy in which spin-diffusion contributions are obtained from the summed contributions of the exact solutions of three-spin systems ijk (Vögeli et al. 2010) for all neighboring spins k within the cross section of the spheres centered at spin i and j. Importantly, scaling the contribution to spin-diffusion from spin k by its protonation level allows the setting of individual, spin specific deuteration levels in sample specific manner corresponding i.e. to methyl-group specific labeling schemes, see
 
The parameter '''b0field''' is the field strength [MHz].
The parameter '''tauc''' is the overall correlation time [ns].  
The parameter '''maxdist''' is the size of the spheres centered at spin i and j.
 
The parameter '''rmode''' is used to specify if experimental or simulated auto-relaxation (rho) values are used.
 
 
The parameter info=full or info=debug may be used to print the simulated buildup values to screen.

Revision as of 15:47, 17 January 2019

Parameters

b0field =real
(default: none)
tauc =real
(default: none)

Description

This converts the calculated cross-correlation rates to distances.

There are two different approaches to determine spin-diffusion contributions to cross-peak buildups, both of which require PDB coordinates of a previously determined structure (a conventional NMR structure or an X-ray structure). Usually the lowest energy model of structure bundles is used for spin-diffusion calculation; however, averaging of spin-diffusion over individual conformers is possible, depending on how many structures were read, see

The parameter mode is used to select the spin diffusion correction method (FRM:1, TSS: 2). For the full-matrix (FRM, mode=1) approach to spin-diffusion approximation we use the multi-spin Solomon equation to express the mixing time-dependence of the NOESY intensities. In the FRM approach, the buildup intensities containing spin-diffusion are calculated for all spins within the spheres centered at spins i and j (Orts et al. 2012).


In the TSS (TSS, mode=2) approach, we follow a strategy in which spin-diffusion contributions are obtained from the summed contributions of the exact solutions of three-spin systems ijk (Vögeli et al. 2010) for all neighboring spins k within the cross section of the spheres centered at spin i and j. Importantly, scaling the contribution to spin-diffusion from spin k by its protonation level allows the setting of individual, spin specific deuteration levels in sample specific manner corresponding i.e. to methyl-group specific labeling schemes, see

The parameter b0field is the field strength [MHz]. The parameter tauc is the overall correlation time [ns]. The parameter maxdist is the size of the spheres centered at spin i and j.

The parameter rmode is used to specify if experimental or simulated auto-relaxation (rho) values are used.


The parameter info=full or info=debug may be used to print the simulated buildup values to screen.